使用tabularray
This commit is contained in:
401
paper/main.tex
401
paper/main.tex
@@ -121,77 +121,75 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
|
|||||||
\begin{sidewaystable}
|
\begin{sidewaystable}
|
||||||
\centering
|
\centering
|
||||||
{
|
{
|
||||||
\newcommand{\twocol}[1]{\multicolumn{2}{C{1cm}|}{#1}}
|
|
||||||
\newcommand{\threecol}[1]{\multicolumn{3}{C{1.5cm}|}{#1}}
|
|
||||||
\newcommand{\wthreecol}[1]{\multicolumn{3}{C{2cm}|}{#1}}
|
|
||||||
\newcommand{\allcol}[1]{\multicolumn{26}{C{16cm}|}{#1}}
|
|
||||||
\setlength\tabcolsep{0pt} % 不加这句话的话，表格的竖线的宽度会被计入，导致合并后的单元格不居中
|
|
||||||
\caption{Weak- and None-polarized phonons near $\Gamma$ point}
|
\caption{Weak- and None-polarized phonons near $\Gamma$ point}
|
||||||
\begin{tabular}{
|
\begin{tblr}{
|
||||||
| C{4cm} % header
|
hlines,vlines,colsep=2pt,width=\textwidth,
|
||||||
| C{0.5cm} | C{0.5cm} | C{0.5cm} % E2
|
colspec={
|
||||||
| C{0.5cm} | C{0.5cm} | C{0.5cm} % E2
|
X[10,c,m]
|
||||||
| C{0.5cm} | C{0.5cm} % E1
|
*{3}{X[c,m]} % E2
|
||||||
| C{1cm} | C{1cm} % 2B1
|
*{3}{X[c,m]} % E2
|
||||||
| C{0.5cm} | C{0.5cm} | C{1cm} % A1
|
*{2}{X[c,m]} % E1
|
||||||
| C{0.5cm} | C{0.5cm} % E1
|
*{2}{X[4,c,m]} % 2B1
|
||||||
| C{0.5cm} | C{0.5cm} | C{0.5cm} % E2
|
*{2}{X[c,m]} X[2,c,m] % A1
|
||||||
| C{0.5cm} | C{0.5cm} | C{0.5cm} % E2
|
*{2}{X[c,m]} % E1
|
||||||
| C{0.5cm} | C{0.5cm} | C{1cm} % A1
|
*{3}{X[c,m]} % E2
|
||||||
| C{1cm} | C{1cm} % 2B1
|
*{3}{X[c,m]} % E2
|
||||||
| }
|
*{2}{X[c,m]} X[2,c,m] % A1
|
||||||
\hline
|
*{2}{X[4,c,m]} % 2B1
|
||||||
\textbf{\makecell{Direction of Incident \\ \& Scattered Light}}
|
}
|
||||||
& \allcol{\makecell{Any direction \\ (not depend on direction of incident \& scattered light)}}
|
}
|
||||||
\\ \hline
|
\textbf{Direction of Incident \& Scattered Light}
|
||||||
|
& \SetCell[c=26]{}{Any direction \\ (not depend on direction of incident \& scattered light)}
|
||||||
|
& & & & & & & & & & & & & & & & & & & & & & & & &
|
||||||
|
\\
|
||||||
\textbf{Number of Phonon}
|
\textbf{Number of Phonon}
|
||||||
& 1 & \twocol{2} % E2
|
& 1 & \SetCell[c=2]{} 2 & % E2
|
||||||
& 3 & \twocol{4} % E2
|
& 3 & \SetCell[c=2]{} 4 & % E2
|
||||||
& 5 & 6 % E1
|
& 5 & 6 % E1
|
||||||
& 7 & 8 % 2B1
|
& 7 & 8 % 2B1
|
||||||
& \wthreecol{9} % A1
|
& \SetCell[c=3]{} 9 & & % A1
|
||||||
& 10 & 11 % E1
|
& 10 & 11 % E1
|
||||||
& 12 & \twocol{13} % E2
|
& 12 & \SetCell[c=2]{} 13 & % E2
|
||||||
& 14 & \twocol{15} % E2
|
& 14 & \SetCell[c=2]{} 15 & % E2
|
||||||
& \wthreecol{16} % A1
|
& \SetCell[c=3]{} 16 & & % A1
|
||||||
& 17 & 18 % 2B1
|
& 17 & 18 % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Vibration Direction}
|
\textbf{Vibration Direction}
|
||||||
& x & \twocol{y} % E2
|
& x & \SetCell[c=2]{} y & % E2
|
||||||
& x & \twocol{y} % E2
|
& x & \SetCell[c=2]{} y & % E2
|
||||||
& x & y % E1
|
& x & y % E1
|
||||||
& z & z % 2B1
|
& z & z % 2B1
|
||||||
& \wthreecol{z} % A1
|
& \SetCell[c=3]{} z & & % A1
|
||||||
& x & y % E1
|
& x & y % E1
|
||||||
& x & \twocol{y} % E2
|
& x & \SetCell[c=2]{} y & % E2
|
||||||
& x & \twocol{y} % E2
|
& x & \SetCell[c=2]{} y & % E2
|
||||||
& \wthreecol{z} % A1
|
& \SetCell[c=3]{} z & & % A1
|
||||||
& z & z % 2B1
|
& z & z % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Representation in Group $\mathrm{C_{6v}}$}
|
\textbf{Representation in Group $\mathrm{C_{6v}}$}
|
||||||
& \threecol{$\mathrm{E_2}$} % E2
|
& \SetCell[c=3]{} $\mathrm{E_2}$ & & % E2
|
||||||
& \threecol{$\mathrm{E_2}$} % E2
|
& \SetCell[c=3]{} $\mathrm{E_2}$ & & % E2
|
||||||
& \twocol{$\mathrm{E_1}$} % E1
|
& \SetCell[c=2]{} $\mathrm{E_1}$ & % E1
|
||||||
& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
|
& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
|
||||||
& \wthreecol{$\mathrm{A_1}$} % A1
|
& \SetCell[c=3]{} $\mathrm{A_1}$ & & % A1
|
||||||
& \twocol{$\mathrm{E_1}$} % E1
|
& \SetCell[c=2]{} $\mathrm{E_1}$ & % E1
|
||||||
& \threecol{$\mathrm{E_2}$} % E2
|
& \SetCell[c=3]{} $\mathrm{E_2}$ & & % E2
|
||||||
& \threecol{$\mathrm{E_2}$} % E2
|
& \SetCell[c=3]{} $\mathrm{E_2}$ & & % E2
|
||||||
& \wthreecol{$\mathrm{A_1}$} % A1
|
& \SetCell[c=3]{} $\mathrm{A_1}$ & & % A1
|
||||||
& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
|
& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Representation in Group $\mathrm{C_{2v}}$}
|
\textbf{Representation in Group $\mathrm{C_{2v}}$}
|
||||||
& $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2
|
& $\mathrm{A_2}$ & \SetCell[c=2]{} $\mathrm{A_1}$ & % E2
|
||||||
& $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2
|
& $\mathrm{A_2}$ & \SetCell[c=2]{} $\mathrm{A_1}$ & % E2
|
||||||
& $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1
|
& $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1
|
||||||
& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
|
& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
|
||||||
& \wthreecol{$\mathrm{A_1}$} % A1
|
& \SetCell[c=3]{} $\mathrm{A_1}$ & & % A1
|
||||||
& $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1
|
& $\mathrm{B_2}$ & $\mathrm{B_1}$ % E1
|
||||||
& $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2
|
& $\mathrm{A_2}$ & \SetCell[c=2]{} $\mathrm{A_1}$ & % E2
|
||||||
& $\mathrm{A_2}$ & \twocol{$\mathrm{A_1}$} % E2
|
& $\mathrm{A_2}$ & \SetCell[c=2]{} $\mathrm{A_1}$ & % E2
|
||||||
& \wthreecol{$\mathrm{A_1}$} % A1
|
& \SetCell[c=3]{} $\mathrm{A_1}$ & & % A1
|
||||||
& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
|
& $\mathrm{B_1}$ & $\mathrm{B_1}$ % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Scattering in Polarization}
|
\textbf{Scattering in Polarization}
|
||||||
& xy & xx & yy % E2
|
& xy & xx & yy % E2
|
||||||
& xy & xx & yy % E2
|
& xy & xx & yy % E2
|
||||||
@@ -203,128 +201,126 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
|
|||||||
& xy & xx & yy % E2
|
& xy & xx & yy % E2
|
||||||
& xx & yy & zz % A1
|
& xx & yy & zz % A1
|
||||||
& - & - % 2B1
|
& - & - % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Raman Intensity (a.u.)}
|
\textbf{Raman Intensity (a.u.)}
|
||||||
& \threecol{$0.17$} % E2
|
& \SetCell[c=3]{} $0.17$ & & % E2
|
||||||
& \threecol{$1.13$} % E2
|
& \SetCell[c=3]{} $1.13$ & & % E2
|
||||||
& \twocol{$2.43$} % E1
|
& \SetCell[c=2]{} $2.43$ & % E1
|
||||||
& $0$ & $0$ % 2B1
|
& $0$ & $0$ % 2B1
|
||||||
& \twocol{$2.83$} & $1.79$ % A1
|
& \SetCell[c=2]{} $2.83$ & & $1.79$ % A1
|
||||||
& \twocol{$0.09$} % E1
|
& \SetCell[c=2]{} $0.09$ & % E1
|
||||||
& \threecol{$88.54$} % E2
|
& \SetCell[c=3]{} $88.54$ & & % E2
|
||||||
& \threecol{$0.50$} % E2
|
& \SetCell[c=3]{} $0.50$ & & % E2
|
||||||
& \twocol{$0.01$} & $1.78$ % A1
|
& \SetCell[c=2]{} $0.01$ & & $1.78$ % A1
|
||||||
& $0$ & $0$ % 2B1
|
& $0$ & $0$ % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Visible in Common Raman Experiment}
|
\textbf{Visible in Common Raman Experiment}
|
||||||
& \threecol{Yes} % E2
|
& \SetCell[c=3]{} Yes & & % E2
|
||||||
& \threecol{Yes} % E2
|
& \SetCell[c=3]{} Yes & & % E2
|
||||||
& \twocol{Yes} % E1
|
& \SetCell[c=2]{} Yes & % E1
|
||||||
& No & No % 2B1
|
& No & No % 2B1
|
||||||
& \wthreecol{Yes} % A1
|
& \SetCell[c=3]{} Yes & & % A1
|
||||||
& \twocol{No} % E1
|
& \SetCell[c=2]{} No & % E1
|
||||||
& \threecol{Yes} % E2
|
& \SetCell[c=3]{} Yes & & % E2
|
||||||
& \threecol{No} % E2
|
& \SetCell[c=3]{} No & & % E2
|
||||||
& \twocol{No} & Yes % A1
|
& \SetCell[c=2]{} No & & Yes % A1
|
||||||
& No & No % 2B1
|
& No & No % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Wavenumber (Simulation) ($\mathrm{cm^{-1}}$)}
|
\textbf{Wavenumber (Simulation) ($\mathrm{cm^{-1}}$)}
|
||||||
& \threecol{$190.51$} % E2
|
& \SetCell[c=3]{} $190.51$ & & % E2
|
||||||
& \threecol{$190.51$} % E2
|
& \SetCell[c=3]{} $190.51$ & & % E2
|
||||||
& \twocol{$257.35$} % E1
|
& \SetCell[c=2]{} $257.35$ & % E1
|
||||||
& $389.96$ & $389.96$ % 2B1
|
& $389.96$ & $389.96$ % 2B1
|
||||||
& \wthreecol{$591.90$} % A1
|
& \SetCell[c=3]{} $591.90$ & & % A1
|
||||||
& \twocol{$746.91$} % E1
|
& \SetCell[c=2]{} $746.91$ & % E1
|
||||||
& \threecol{$756.25$} % E2
|
& \SetCell[c=3]{} $756.25$ & & % E2
|
||||||
& \threecol{$764.33$} % E2
|
& \SetCell[c=3]{} $764.33$ & & % E2
|
||||||
& \wthreecol{$812.87$} % A1
|
& \SetCell[c=3]{} $812.87$ & & % A1
|
||||||
& $885.68$ & $894.13$ % 2B1
|
& $885.68$ & $894.13$ % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Wavenumber (Experiment) ($\mathrm{cm^{-1}}$)}
|
\textbf{Wavenumber (Experiment) ($\mathrm{cm^{-1}}$)}
|
||||||
& \threecol{$195.5$} % E2
|
& \SetCell[c=3]{} $195.5$ & & % E2
|
||||||
& \threecol{$203.3$} % E2
|
& \SetCell[c=3]{} $203.3$ & & % E2
|
||||||
& \twocol{$269.7$} % E1
|
& \SetCell[c=2]{} $269.7$ & % E1
|
||||||
& - & - % 2B1
|
& - & - % 2B1
|
||||||
& \wthreecol{$609.5$} % A1
|
& \SetCell[c=3]{} $609.5$ & & % A1
|
||||||
& \twocol{-} % E1
|
& \SetCell[c=2]{} - & % E1
|
||||||
& \threecol{$776$} % E2
|
& \SetCell[c=3]{} $776$ & & % E2
|
||||||
& \threecol{-} % E2
|
& \SetCell[c=3]{} - & & % E2
|
||||||
& \twocol{-} & $839$ % A1
|
& \SetCell[c=2]{} - & $839$ % A1
|
||||||
& - & - % 2B1
|
& - & - % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Electrical Polarity}
|
\textbf{Electrical Polarity}
|
||||||
& \threecol{None} % E2
|
& \SetCell[c=3]{} None & & % E2
|
||||||
& \threecol{None} % E2
|
& \SetCell[c=3]{} None & & % E2
|
||||||
& \twocol{Weak} % E1
|
& \SetCell[c=2]{} Weak & % E1
|
||||||
& None & None % 2B1
|
& None & None % 2B1
|
||||||
& \wthreecol{Weak} % A1
|
& \SetCell[c=3]{} Weak & & % A1
|
||||||
& \twocol{Weak} % E1
|
& \SetCell[c=2]{} Weak & % E1
|
||||||
& \threecol{None} % E2
|
& \SetCell[c=3]{} None & & % E2
|
||||||
& \threecol{None} % E2
|
& \SetCell[c=3]{} None & & % E2
|
||||||
& \wthreecol{Weak} % A1
|
& \SetCell[c=3]{} Weak & & % A1
|
||||||
& None & None % 2B1
|
& None & None % 2B1
|
||||||
\\ \hline
|
\\
|
||||||
\end{tabular}
|
\end{tblr}
|
||||||
}
|
}
|
||||||
{
|
{
|
||||||
\newcommand{\tworow}[1]{\multirow{2}{*}{#1}}
|
|
||||||
\newcommand{\twocol}[2]{\multicolumn{2}{C{#1}|}{#2}}
|
|
||||||
\newcommand{\threecol}[2]{\multicolumn{3}{C{#1}|}{#2}}
|
|
||||||
\newcommand{\fourcol}[1]{\multicolumn{4}{C{2cm}|}{#1}}
|
|
||||||
\setlength\tabcolsep{0pt} % 不加这句话的话，表格的竖线的宽度会被计入，导致合并后的单元格不居中
|
|
||||||
\caption{Strong-polarized phonons near $\Gamma$ point}
|
\caption{Strong-polarized phonons near $\Gamma$ point}
|
||||||
\begin{tabular}{
|
\begin{tblr}{
|
||||||
| C{4cm} % header
|
hlines,vlines,colsep=2pt,width=\textwidth,hspan=even,
|
||||||
| C{1cm} | C{1cm} % z E1
|
colspec={
|
||||||
| C{0.7cm} | C{0.7cm} | C{1cm} % z A1
|
X[5,c,m]
|
||||||
| C{0.5cm} | C{0.5cm} | C{0.5cm} % y z
|
X[c,m] % z x
|
||||||
| C{1cm} % y x
|
X[c,m] % z y
|
||||||
| C{1cm} % y y
|
*{2}{X[c,m]}X[c,m,1.5] % z z
|
||||||
| C{0.5cm} | C{0.5cm} | C{0.5cm} | C{0.5cm} % 45 y&z mainly z
|
X[c,m,2]X[c,m]X[c,m,2] % y z
|
||||||
| C{1cm} % 45 x
|
X[c,m,1.5] % y x
|
||||||
| C{0.5cm} | C{0.5cm} | C{0.5cm} | C{0.5cm} % 45 y&z mainly y
|
X[c,m,2] % y y
|
||||||
| }
|
*{3}{X[c,m]}X[c,m,1.5] % 45 y&z mainly z
|
||||||
\hline
|
X[c,m,1.5] % 45 x
|
||||||
|
*{4}{X[c,m]} % 45 y&z mainly y
|
||||||
|
}
|
||||||
|
}
|
||||||
\textbf{Direction of Incident \& Scattered Light}
|
\textbf{Direction of Incident \& Scattered Light}
|
||||||
& \multicolumn{5}{C{4cm}|}{z}
|
& \SetCell[c=5]{} z & & & &
|
||||||
& \multicolumn{5}{C{3.9cm}|}{y}
|
& \SetCell[c=5]{} y & & & &
|
||||||
& \multicolumn{9}{C{5cm}|}{between z and y, 10\textdegree{} to z}
|
& \SetCell[c=9]{} between z and y, 10\textdegree{} to z & & & & & & & &
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Number of Phonon}
|
\textbf{Number of Phonon}
|
||||||
& 1 & 2 % z E1
|
& 1 & 2 % z E1
|
||||||
& \threecol{2.4cm}{3} % z A1
|
& \SetCell[c=3]{} 3 & & % z A1
|
||||||
& \threecol{1.5cm}{1} % y z
|
& \SetCell[c=3]{} 1 & & % y z
|
||||||
& 2 % y x
|
& 2 % y x
|
||||||
& 3 % y y
|
& 3 % y y
|
||||||
& \fourcol{1} % 45 y&z mainly z
|
& \SetCell[c=4]{} 1 & & & % 45 y&z mainly z
|
||||||
& 2 % 45 x
|
& 2 % 45 x
|
||||||
& \fourcol{3} % 45 y&z mainly y
|
& \SetCell[c=4]{} 3 & & & % 45 y&z mainly y
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Vibration Direction}
|
\textbf{Vibration Direction}
|
||||||
& x (TO) & y (TO) % z E1
|
& {x \\ (TO)} & {y \\ (TO)} % z E1
|
||||||
& \threecol{2.4cm}{z (LO)} % z A1
|
& \SetCell[c=3]{} z (LO) & & % z A1
|
||||||
& \threecol{1.5cm}{z (TO)} % y z
|
& \SetCell[c=3]{} z (TO) & & % y z
|
||||||
& x (TO) % y x
|
& {x \\ (TO)} % y x
|
||||||
& y (LO) % y y
|
& {y \\ (LO)} % y y
|
||||||
& \fourcol{y-z mixed (LO-TO mixed)} % 45 y&z mainly z
|
& \SetCell[c=4]{} {y-z mixed \\ (LO-TO mixed)} & & & % 45 y&z mainly z
|
||||||
& x (TO) % 45 x
|
& x (TO) % 45 x
|
||||||
& \fourcol{y-z mixed (LO-TO mixed)} % 45 y&z mainly y
|
& \SetCell[c=4]{} {y-z mixed \\ (LO-TO mixed)} & & & % 45 y&z mainly y
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Representation in Group $\mathrm{C_{6v}}$}
|
\textbf{Representation in Group $\mathrm{C_{6v}}$}
|
||||||
& \twocol{2cm}{$\mathrm{E_1}$}
|
& \SetCell[c=2]{} $\mathrm{E_1}$ &
|
||||||
& \threecol{2.4cm}{$\mathrm{A_1}$}
|
& \SetCell[c=3]{} $\mathrm{A_1}$ & &
|
||||||
& \multicolumn{14}{C{8.5cm}|}{Not applicable}
|
& \SetCell[c=14]{} Not applicable & & & & & & & & & & & & &
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Representation in Group $\mathrm{C_{2v}}$}
|
\textbf{Representation in Group $\mathrm{C_{2v}}$}
|
||||||
& $\mathrm{B_2}$ & $\mathrm{B_1}$ % z E1
|
& $\mathrm{B_2}$ & $\mathrm{B_1}$ % z E1
|
||||||
& \threecol{2.4cm}{$\mathrm{A_1}$} % z A1
|
& \SetCell[c=3]{} $\mathrm{A_1}$ & & % z A1
|
||||||
& \threecol{1.5cm}{$\mathrm{A_1}$} % y z
|
& \SetCell[c=3]{} $\mathrm{A_1}$ & & % y z
|
||||||
& $\mathrm{B_2}$ % y x
|
& $\mathrm{B_2}$ % y x
|
||||||
& $\mathrm{B_1}$ % y y
|
& $\mathrm{B_1}$ % y y
|
||||||
& \fourcol{Not Applicable} % 45 y&z mainly z
|
& \SetCell[c=4]{} Not Applicable & & & % 45 y&z mainly z
|
||||||
& $\mathrm{B_2}$ % 45 x
|
& $\mathrm{B_2}$ % 45 x
|
||||||
& \fourcol{Not Applicable} % 45 y&z mainly y
|
& \SetCell[c=4]{} Not Applicable & & & % 45 y&z mainly y
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Scattering in Polarization}
|
\textbf{Scattering in Polarization}
|
||||||
& xz & yz % z E1
|
& xz & yz % z E1
|
||||||
& xx & yy & zz % z A1
|
& xx & yy & zz % z A1
|
||||||
@@ -334,40 +330,39 @@ Thus, we divide the phonons of defect-free 4H-SiC into three categories:
|
|||||||
& xx & yy & yz & zz % 45 y&z mainly z
|
& xx & yy & yz & zz % 45 y&z mainly z
|
||||||
& xz % 45 x
|
& xz % 45 x
|
||||||
& xx & yy & yz & zz % 45 y&z mainly y
|
& xx & yy & yz & zz % 45 y&z mainly y
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Raman Intensity (a.u.)}
|
\textbf{Raman Intensity (a.u.)}
|
||||||
& \twocol{2cm}{$53.52$} % z E1
|
& \SetCell[c=2]{} $53.52$ & % z E1
|
||||||
& \twocol{1.4cm}{$53.52$} & $464.69$ % z A1
|
& \SetCell[c=2]{} $53.52$ & & $464.69$ % z A1
|
||||||
& \twocol{1cm}{$56.86$} & $454.09$ % y z
|
& \SetCell[c=2]{} $56.86$ & & $454.09$ % y z
|
||||||
& $53.52$ % y x
|
& $53.52$ % y x
|
||||||
& $53.55$ % y y
|
& $53.55$ % y y
|
||||||
& \twocol{1cm}{$53.71$} & $3.20$ & $425.98$ % 45 y&z mainly z
|
& \SetCell[c=2]{} $53.71$ & & $3.20$ & $425.98$ % 45 y&z mainly z
|
||||||
& $53.56$ % 45 x
|
& $53.56$ % 45 x
|
||||||
& \twocol{1cm}{$3.60$} & $50.36$ & $27.99$ % 45 y&z mainly y
|
& \SetCell[c=2]{} $3.60$ & & $50.36$ & $27.99$ % 45 y&z mainly y
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Visible in Common Raman Experiment}
|
\textbf{Visible in Common Raman Experiment}
|
||||||
& \twocol{2cm}{Yes} % z E1
|
& \SetCell[c=2]{} Yes & % z E1
|
||||||
& \twocol{1.4cm}{Yes (LOPC)} & No % z A1
|
& \SetCell[c=2]{} {Yes \\ (LOPC)} & & No % z A1
|
||||||
& Yes (overfocused) & No & Yes (overfocused) % y z
|
& Yes (overfocused) & No & Yes (overfocused) % y z
|
||||||
& Yes % y x
|
& Yes % y x
|
||||||
& Yes (LOPC) % y y
|
& {Yes \\ (LOPC)} % y y
|
||||||
& \fourcol{???} % 45 y&z mainly z
|
& \SetCell[c=4]{} ??? & & & % 45 y&z mainly z
|
||||||
& ??? % 45 x
|
& ??? % 45 x
|
||||||
& \fourcol{???} % 45 y&z mainly y
|
& \SetCell[c=4]{} ??? & & & % 45 y&z mainly y
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Wavenumber (Simulation) ($\mathrm{cm^{-1}}$)}
|
\textbf{Wavenumber (Simulation) ($\mathrm{cm^{-1}}$)}
|
||||||
& \twocol{2cm}{$776.57$} % z E1
|
& \SetCell[c=2]{} $776.57$ & % z E1
|
||||||
& \threecol{2.4cm}{$933.80$} % z A1
|
& \SetCell[c=3]{} $933.80$ & & % z A1
|
||||||
& \threecol{1.5cm}{$761.80$} % y z
|
& \SetCell[c=3]{} $761.80$ & & % y z
|
||||||
& $776.57$ % y x
|
& $776.57$ % y x
|
||||||
& $941.33$ % y y
|
& $941.33$ % y y
|
||||||
& \fourcol{$762.76$} % 45 y&z mainly z
|
& \SetCell[c=4]{} $762.76$ & & & % 45 y&z mainly z
|
||||||
& $776.57$ % 45 x
|
& $776.57$ % 45 x
|
||||||
& \fourcol{$940.86$} % 45 y&z mainly y
|
& \SetCell[c=4]{} $940.86$ & & & % 45 y&z mainly y
|
||||||
\\ \hline
|
\\
|
||||||
\textbf{Electrical Polarity} & \multicolumn{19}{C{12.9cm}|}{Strong}
|
\textbf{Electrical Polarity} & \SetCell[c=19]{} Strong & & & & & & & & & & & & & & & & & &
|
||||||
\\ \hline
|
\end{tblr}
|
||||||
\end{tabular}
|
|
||||||
}
|
}
|
||||||
\label{tab:phonon}
|
\label{tab:phonon}
|
||||||
\end{sidewaystable}
|
\end{sidewaystable}
|
||||||
|
|||||||
Reference in New Issue
Block a user